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1.
The paper deals with orthogonal polynomials in the case where the orthogonality condition is related to semiclassical functionals. The polynomials that we discuss are a generalization of Jacobi polynomials and Jacobi-type polynomials. More precisely, we study some algebraic properties as well as the asymptotic behaviour of polynomials orthogonal with respect to the linear functional U U=J ,+A 1(x–1)+B 1(x+1)–A 2(x–1)–B 2(x+1), where J , is the Jacobi linear functional, i.e. J ,,p›=–1 1 p(x)(1–x)(1+x)dx,,>–1, pP, and P is the linear space of polynomials with complex coefficients. The asymptotic properties are analyzed in (–1,1) (inner asymptotics) and C[–1,1] (outer asymptotics) with respect to the behaviour of Jacobi polynomials. In a second step, we use the above results in order to obtain the location of zeros of such orthogonal polynomials. Notice that the linear functional U is a generalization of one studied by T. H. Koornwinder when A 2=B 2=0. From the point of view of rational approximation, the corresponding Markov function is a perturbation of the Jacobi–Markov function by a rational function with two double poles at ±1. The denominators of the [n–1/n] Padé approximants are our orthogonal polynomials.  相似文献   

2.
Guyan Robertson 《K-Theory》2001,22(3):251-269
Let be a torsionfree lattice in G=PGL(n+1, , where n 1 and is a nonArchimedean local field. Then acts on the Furstenberg boundary G/P, where P is a minimal parabolic subgroup of G. The identity element I in the crossedproduct C *algebra C(G/P) generates a class [I] in the K 0 group of C(G/P) . It is shown that [I] is a torsion element of K 0 and there is an explicit bound for the order of [I]. The result is proved more generally for groups acting on affine buildings of type à n. For n=1, 2 the Euler–Poincaré characteristic () annihilates the class [I].  相似文献   

3.
We evaluate finite-temperature equilibrium correlators for thermal time ordered Bose fields to good approximations by new methods of functional integration in d=1,2,3 dimensions and with the trap potentials V(r)0. As in the translationally invariant cases, asymptotic behaviors fall as to longer-range condensate values for and only for d=3 in agreement with experimental observations; but there are generally significant corrections also depending on due to the presence of the traps. For d=1, we regain the exact translationally invariant results as the trap frequencies 0. In analyzing the attractive cases, we investigate the time-dependent c-number Gross–Pitaevskii (GP) equation with the trap potential for a generalized nonlinearity –2c||2n and c<0. For n=1, the stationary form of the GP equation appears in the steepest-descent approximation of the functional integrals. We show that collapse in the sense of Zakharov can occur for c=0 and nd2 and a functional E NLS[]0 even when V(r)0. The singularities typically arise as -functions centered on the trap origin r=0.  相似文献   

4.
In this paper we show the strong mean square convergence of a numerical scheme for a R d -multivalued stochastic differential equation: dX t +A(X t )dtb(t,X t )dt+(t,X t )dW t and obtain the rate of convergence O(( log(1/)1/2) when the diffusion coefficient is bounded. By introducing a discrete Skorokhod problem, we establish L p -estimates (p2) for the solutions and prove the convergence by using a deterministic result. Numerical experiments for the rate of convergence are presented.  相似文献   

5.
We obtain the analytic expression for the total cross section of the reaction e e +l l + (l=,) taking possible quasianapole interaction effects into account. We find numerical restrictions on the interaction parameter value from data for the reaction e e ++ in the energy domain below the Z 0 peak.  相似文献   

6.
We consider solutions of the class of ODEs y=6y 2x , which contains the first Painlevé equation (PI) for =1. It is well known that PI has a unique real solution (called a tritronquée solution) asymptotic to and decaying monotonically on the positive real line. We prove the existence and uniqueness of a corresponding solution for each real nonnegative 1.  相似文献   

7.
The paper studies singular eigenvalue problems for the equation y (n) +p(x)y=0 with boundary conditions imposed on the derivatives y (i) at the points x=a and x=. We look for singular problems which are analogous to regular problems on a finite interval. It is characterized when each eigenfunction has a finite number of zeros and when the spectrum is discrete or continuous, respectively.  相似文献   

8.
For eachk andd, 1kd, definef(d, d)=d+1 andf(d, k)=2d if 1kd–1. The following results are established:Let be a uniformly bounded collection of compact, convex sets inR d . For a fixedk, 1kd, dim {MM in }k if and only if for some > 0, everyf(d, k) members of contain a commonk-dimensional set of measure (volume) at least.LetS be a bounded subset ofR d . Assume that for some fixedk, 1kd, there exists a countable family of (k–l)-flats {H i :i1} inR d such that clS S {Hi i 1 } and for eachi1, (clS S) H i has (k–1) dimensional measure zero. Every finite subset ofS sees viaS a set of positivek-dimensional measure if and only if for some>0, everyf(d,k) points ofS see viaS a set ofk-dimensional measure at least .The numbers off(d,d) andf(d, 1) above are best possible.Supported in part by NSF grant DMS-8705336.  相似文献   

9.
Let G be a connected reductive algebraic group over an algebraically closed field k of characteristic p0, and =LieG. In positive characteristic, suppose in addition that p is good for G and the derived subgroup of G is simply connected. Let =() denote the nilpotent variety of , and nil():={(x,y)×|[x,y]=0}, the nilpotent commuting variety of . Our main goal in this paper is to show that the variety nil() is equidimensional. In characteristic 0, this confirms a conjecture of Vladimir Baranovsky; see [2]. When applied to GL(n), our result in conjunction with an observation in [2] shows that the punctual (local) Hilbert scheme n Hilb n (2) is irreducible over any algebraically closed field. Mathematics Subject Classification (2000) 20G05  相似文献   

10.
We argue extensively in favor of our earlier choice of the in and out states (among the solutions of a wave equation with one-dimensional potential). In this connection, we study the nonstationary and stationary families of complete sets of solutions of the Klein–Gordon equation with a constant electric field. A nonstationary set Pv consists of the solutions with the quantum number p v=p 0 v–p3. It can be obtained from the nonstationary set P3 with the quantum number p 3 by a boost along the x 3 axis (in the direction of the electric field) with the velocity –v. By changing the gauge, we can bring the solutions in all sets to the same potential without changing quantum numbers. Then the transformations of solutions in one set (with the quantum number p v) to the solutions in another set (with the quantum number p v) have group properties. The stationary solutions and sets have the same properties as the nonstationary ones and are obtainable from stationary solutions with the quantum number p 0 by the same boost. It turns out that each set can be obtained from any other by gauge manipulations. All sets are therefore equivalent, and the classification (i.e., assigning the frequency sign and the in and out indices) in any set is determined by the classification in the set P3, where it is obvious.  相似文献   

11.
G. Sartori  G. Valente 《Acta Appl Math》2005,87(1-3):191-228
We review the proposal of a constructive axiomatic approach to the determination of the orbit spaces of all the real compact linear groups, obtained through the computation of a metric matrix , which is defined only in terms of the scalar products between the gradients p1(x),...,pq(x) of the elements of a minimal integrity basis (MIB) for the ring [n]G of G-invariant polynomials. The domain of semi-positivity of is known to realize the orbit space n/G of G as a semi-algebraic variety in the space q spanned by the variables p1,...,pq. The matrices can be obtained from the solutions of a universal differential equation (master equation), which satisfy convenient initial conditions. The master equation and the initial conditions involve as free parameters only the degrees da of the pa(x)s. This approach tries to bypass the actual impossibility of explicitly determining a set of basic polynomial invariants for each group. Our results may be relevant in physical contexts where the study of covariant or invariant functions is important, like in the determination of patterns of spontaneous symmetry breaking in quantum field theory, in the analysis of phase spaces and structural phase transitions (Landaus theory), in covariant bifurcation theory, in crystal field theory and so on. Mathematics Subject Classifications (2000) 14L24, 13A50, 14L30.This paper is partially supported by INFN and MURST 40% and 60%.  相似文献   

12.
Let X/Fp be an Artin–Schreier curve defined by the affine equation y p y=f(x) where f(x)Fp[x] is monic of degree d. In this paper we develop a method for estimating the first slope of the Newton polygon of X. Denote this first slope by NP1(X/Fp). We use our method to prove that if p>d2 then NP1(X/Fp)(p–1)/d/(p–1). If p>2d4, we give a sufficient condition for the equality to hold.  相似文献   

13.
R. Alexander 《Combinatorica》1990,10(2):115-136
Let be a signed measure on E d with E d =0 and ¦¦Ed<. DefineD s() as sup ¦H¦ whereH is an open halfspace. Using integral and metric geometric techniques results are proved which imply theorems such as the following.Theorem A. Let be supported by a finite pointsetp i. ThenD s()>c d(1/ 2)1/2{ i(p i)2}1/2 where 1 is the minimum distance between two distinctp i, and 2 is the maximum distance. The numberc d is an absolute dimensional constant. (The number .05 can be chosen forc 2 in Theorem A.)Theorem B. LetD be a disk of unit area in the planeE 2, andp 1,p 2,...,p n be a set of points lying inD. If m if the usual area measure restricted toD, while nP i=1/n defines an atomic measure n, then independently of n,nD s(m n) .0335n 1/4. Theorem B gives an improved solution to the Roth disk segment problem as described by Beck and Chen. Recent work by Beck shows thatnD s(m n)cn 1/4(logn)–7/2.  相似文献   

14.
We consider the Hamiltonian H (K) of a system consisting of three bosons that interact through attractive pair contact potentials on a three-dimensional integer lattice. We obtain an asymptotic value for the number N(K,z) of eigenvalues of the operator H0(K) lying below z0 with respect to the total quasimomentum K0 and the spectral parameter z–0.  相似文献   

15.
Summary If 1, ... , are non-atomic probability measures on the same measurable space (S, ), then there is an -measurable partition {A i } i = 1 n of S so that i (A i )(n – 1 + m)–1 for all i=1, ..., n, where is the total mass of the largest measure dominated by each of the i S; moreover, this bound is attained for all n1 and all m in [0, 1]. This result is an analog of the bound (n+1-M) -1of Elton et al. [5] based on the mass M of the supremum of the measures; each gives a quantative generalization of a well-known cake-cutting inequality of Urbanik [10] and of Dubins and Spanier [2].Research partly supported by NSF Grants DMS-84-01604 and DMS-86-01608  相似文献   

16.
Let be a positive Radon measure in R n with compact support . Let Q jm be cubes with side-length 2-j+1 originating from the canonical tiling of R n where j\in N 0 and m\in Z n. If \in R, 0 < p \le , 0 < q \le , then pq is the mixed q p -quasi-norm of the sequence 2 j (Q jm ). Quantities of this type are considered in fractal geometry (multifractal formalism) and in the theory of the function spaces B s pq (R n) and F s pq (R n). In Theorem 1 we deal with the question when pq is an equivalent quasi-norm in some of these spaces (-property). If || = 0, then S consists of those points (t,s) in the ts-diagram in Figure 1 for which belongs to B s p (R n) with pt = 1. Theorem 2 deals with the interrelation of S and pq . Some applications to truncated Riesz potentials, Bessel potentials and Fourier transforms of are given.  相似文献   

17.
For a Riemannian manifold Mn with the curvature tensor R, the Jacobi operator RX is defined by RXY=R(X,Y)X. The manifold Mn is called pointwise Osserman if, for every pMn, the eigenvalues of the Jacobi operator RX do not depend of a unit vector XTpMn, and is called globally Osserman if they do not depend of the point p either. R. Osserman conjectured that globally Osserman manifolds are flat or locally rank-one symmetric. This Conjecture is true for manifolds of dimension n8,16[14]. Here we prove the Osserman Conjecture and its pointwise version for 8-dimensional manifolds.Mathematics Subject Classification (2000): 53B20  相似文献   

18.
19.
Using a capacity approach, we prove in this article that it is always possible to define a realization of the Laplacian on L 2() with generalized Robin boundary conditions where is an arbitrary open subset of R n and is a Borel measure on the boundary of . This operator generates a sub-Markovian C 0-semigroup on L 2(). If d=d where is a strictly positive bounded Borel measurable function defined on the boundary and the (n–1)-dimensional Hausdorff measure on , we show that the semigroup generated by the Laplacian with Robin boundary conditions has always Gaussian estimates with modified exponents. We also obtain that the spectrum of the Laplacian with Robin boundary conditions in L p () is independent of p[1,). Our approach constitutes an alternative way to Daners who considers the (n–1)-dimensional Hausdorff measure on the boundary. In particular, it allows us to construct a conterexample disproving Daners' closability conjecture.  相似文献   

20.
We call an R d -valued stochastic process X t with characteristic function exp{–t{(m 2/+2)/2m}},R d ,m>0, the relativistic -stable process. In the paper we derive sharp estimates for the Green function of the relativistic -stable process on C 1,1 domains. Using these estimates we provide lower and upper bounds for the Poisson kernel. As another application we derive 3G Theorem and Boundary Harnack Principle for C 1,1 domains.  相似文献   

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